Discontinuous Galerkin method for two-dimensional bilayer shallow water equations
Electrolyte Gated Organic Field-Effect Transistor Sensors Based on Supported Biotinylated...
Transcript of Electrolyte Gated Organic Field-Effect Transistor Sensors Based on Supported Biotinylated...
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adma201203587 10.1002/adma.201203587
CommunicationsCommunicationsSensorsSensors
M. Magliulo, A.Mallardi, Mohd. Y.Mulla, S. Cotrone, B.R. Pistillo, P. F.Vikholm-Lundin, G.Palazzo, L. Torsi............x‒xx
Anchored,Anchored,biotinylated biotinylated [PE-[PE-Q1:AU]Q1:AU] Definit ion?Definit ion? PLsPLsforming the capturinglayers in an electrolyte-gated organic field-effecttransistor (EGOFET)allow label-freeelectronic specificdetection at aconcentration level of 10nM in a high ionicstrength solution. Thesensing mechanism isbased on a [PE-[PE-Q2:AU]Q2:AU] would "strong"would "strong"or maybe "clear" beor maybe "clear" bebetter here?better here? neatcapacitive effect acrossthe PL layers involvingthe charges of the targetmolecules.
Electrolyte-GatedElectrolyte-GatedOrganic Field-Organic Field-Effect TransistorEffect TransistorSensors BasedSensors Basedon Supportedon SupportedBiotinylatedBiotinylatedPhospholipidPhospholipidBilayerBilayer
Electrolyte-Gated Organic Field-EffectElectrolyte-Gated Organic Field-EffectTransistor Sensors Based on SupportedTransistor Sensors Based on SupportedBiotinylated Phospholipid BilayerBiotinylated Phospholipid Bilayer [PE-Q3:AU][PE-Q3:AU] Tit leTit le
reduced in length sl ight ly to make i t more concise. Ok?reduced in length sl ight ly to make i t more concise. Ok?
By Maria Magliulo1 Antonia Mallardi2 Mohammad Yusuf Mulla1 SerafinaCotrone1 Bianca Rita Pistillo1 Pietro Favia1 Inger Vikholm-Lundin3 Gerardo
Palazzo1,* and Luisa Torsi1,*
1M. Magliulo, M. Y. Mulla, S. Cotrone, B. R. Pistillo, P. Favia, G. Palazzo, L. Torsi,Dipartimento di Chimica, Università degli Studi di Bari Aldo Moro, Via Orabona 4,70126, Bari, Italy; E-mail: [email protected]; [email protected] [PE-[PE-
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Q4:AU]Q4:AU] Please provide academic t i t les for al l authors, i .e., Prof. or Dr.Please provide academic t i t les for al l authors, i .e., Prof. or Dr.
2A. Mallardi, CNR-IPCF, Istituto per i Processi Chimico-Fisici Via Orabona 4,70126, Bari, Italy [PE-Q5:AU][PE-Q5:AU] Please provide academic t i t les for al l authors, i .e., Prof. or Dr.Please provide academic t i t les for al l authors, i .e., Prof. or Dr.
3I. Vikholm-Lundin, VTT Technical Research Centre of Finland, Sinitaival 6, FI-33101 Tampere, Finland [PE-Q6:AU][PE-Q6:AU] Please provide academic t i t les for al l authors, i .e.,Please provide academic t i t les for al l authors, i .e.,
Prof. or Dr.Prof. or Dr.
*Correspondence to: G. Palazzo (E-mail: [email protected]); L. Torsi (E-mail: [email protected])
Received: 08-28-2012 ; Revised: 11-05-2012 ; Published online: MM-DD-YYYY
KeywordsKeywordselectronic sensing, organic field-effect transistors, electrolyte-gated organic field-effect transistors
There is an increasing interest in low cost, timesaving, yet reliable, point-of-care assays. Direct
electronic, label-free transduction of bio-recognition events represents a compelling alternative
offering miniaturization, easy data handling and processing. Low costs and versatility [PE-[PE-
Q7:AU]Q7:AU] Reworded for language clari ty. Original meaning retained?Reworded for language clari ty. Original meaning retained? can be provided if organic electronic
devices such as organic field-effect transistors (OFETs) are used as transducers.[1,2] At the
beginning, OFET sensors mostly involved the detection of volatile chemical analytes,[3,4] while
organic electronics allowed fabrication of sensing circuits on flexible substrates.[5,6] However,
bare OFET-sensor responses are based on weak interactions that are non-specific in nature.
Specificity can be achieved by endowing the OFET with receptor molecules capable of selectively
interacting with given analytes. One of the first successful examples, involving a bi-layer structure
formed by a chiral-active layer deposited on top of an organic semiconductor (OSC), has allowed
electronic, chiral differential detection at an unprecedented low concentration.[7]
Mother Nature is an endless source of specific interactions as recognition events are the basis
of life. Accordingly, the challenge is now to develop OFET bio-sensors by integrating
biomolecules into the transistor device.[8] To date, the three architectures shown on the left side
of Figure 1Figure 1, have been proposed.
Figure 1Figure 1 Schemes of the architectures of OFET biosensors proposed to date: a) bi-layer OFET; b)
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functional biological interlayer (FBI) OFET; c) electrolyte-gated OFET (EGOFET). d) Scheme ofphospholipid BIOEGOFET fabrication. e) Typical source-drain current-voltage characteristics (black curves,left ordinate) and gate currents (red curves, right ordinate) of a BIOEGOFET in presence of [PE-[PE-
Q8:AU]Q8:AU] Definit ion ok?Definit ion ok? phosphate-buffered saline (PBS). [PE-Q9:AU][PE-Q9:AU] Author please ignore this query.Author please ignore this query.
Typesetters: Please ensure this f igure spreads across 1.3 columns.Typesetters: Please ensure this f igure spreads across 1.3 columns.
The first one exploits the already introduced bi-layer structure (Figure 1a) with the receptors
anchored at the OSC surface where an aqueous sample is placed. The use of an ultra-thin
polymer dielectric gate allows for convenient sub-volt operation.[9-11]
A second architecture (Figure 1b) is the functional bio-interlayer (FBI) OFET[12] example,
where the bio-receptor layer is located between the OSC and the gate dielectric, opportunely in
direct contact with the transistor electronic channel. Such an arrangement is the key for
unprecedented sensitivity along with selectivity. A drawback is that the analyte has to percolate
through the OSC to reach the receptors, and while this takes place efficiently for species with low
molecular weights such as insulin, it could be hindered for larger protein complexes or viruses.
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A third configuration (Figure 1c) applies to the electrochemical OFET (ECT)[13-15] and the
electrolyte-gated OFET (EGOFET),[16-18] the former being limited to the detection of
electrochemically active species. In EGOFETs, the dielectric gating is achieved through the
formation of a Debye‒Helmholtz double layer (a few angstroms thickness) at the interface
between the electrolyte solution and the OSC layer (capacitance of the order of 10 μF cm-2)
allowing for sub-volt operation.[19] On the other hand, operation in pure water has been generally
proposed to minimize the electrochemical doping of the OSC in EGOFETs.[20] In ECTs and
EGOFETs the bio-receptor layer overlies the transistor channel, thus the architectures in Figure
1a and Figure 1c share the problem of efficiently grafting recognition bio-elements, hydrophilic in
nature, to the OSC [PE-Q10:AU][PE-Q10:AU] correct now?correct now? which is notably highly hydrophobic. Such a process
generally involves the presence of polar anchoring groups such as hydroxyl, carboxyl, and amino
groups, covalently bound to the OSC backbone. Indeed, the chemical synthesis of a poly(3-
hexylthiophene) (P3HT) derivative bearing carboxylic acid moieties was recently proposed to
achieve DNA covalent linkage to an EGOFET configuration.[21] Changes upon hybridization with
complementary strands in the 0.1 μM concentration range were detected in pure water while no
signal could be detected in saline solution, this occurrence clearly limiting the use of EGOFETs
for biosensing in real samples. Besides, the presence of polar groups in the bulk of a OSC, has
an impact on the transistor performance even when blends are used.[22]
This work presents a general platform for EGOFET biosensing demonstrating that proper bio-
functionalization can lead to stable and reliable label-free electronic sensing in electrolyte solution
with physiologically relevant ionic strength. This is achieved by anchoring, just at the OSC
surface, a capturing bio-layer capable of controlling ionic diffusion into the OSC. The EGOFET
biological functionalization is shown in Figure 1d (see Experimental for more details). The OSC
surface modification is achieved by plasma enhanced vapor chemical deposition (PE-CVD)[23,24]
recently proposed for configurations 1a[10] and 1c.[25] In the latter the PE-CVD, allowing
deposition of a few nanometer-thick-coating rich in COOH groups (Step 1, Figure 1d), has
already been proven to minimally affect the EGOFET electronic performances. These COOH
groups are eventually used to stably anchor phospholipid (PL) molecules, to the OSC surface.
PLs have been chosen as they are versatile bio-systems, being the main components of
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biological membranes; they are amphipathic molecules, i.e., endowed with both hydrophilic and
hydrophobic moieties, that spontaneously self-assemble in water, forming bilayers facing the
outer aqueous domains with their hydrophilic moiety (the PL head) and, secluding in the interior of
the bilayer, the two hydrophobic acyl chains (the PL tails). Being formed by an non-polar oil-like
inner part, the PL bilayers hold a capacitance of around 1 μF cm-2.[26] Under suitable conditions,
the bilayers in water close themselves forming spherical PL shells known as vesicles. Such
vesicles, containing a fraction of PL-bearing amino groups or biotin (biotinylated PL), are prepared
and immobilized (step 2) at the OSC surface through the formation of amide bonds between the
COOH and the PLs amino groups. Eventually, the anchored vesicles spontaneously fuse,
leading to the formation of a PL bilayer stably grafted at the OSC surface (step 3 of Figure 1d).
The non-polar nature of the deposited PL bilayer interior minimizes ionic diffusion through the
membrane, eventually limiting the OSC doping,[27] while the biotinylated PLs conveniently furnish
the binding sites for streptavidin- or avidin-capturing proteins.
Such a bio-modified EGOFET (hereafter called BIOEGOFET) retains good field-effect
performance, as shown by the current‒voltage characteristics (Figure 1e) measured in
phosphate- buffered saline (PBS) solution (10 mM, pH = 7.4) with high ionic strength (0.15 M).
The source-drain current IDS exhibits well shaped linear and saturation regions as the source-
drain bias (VDS) is swept, showing also good modulation with the gate bias VG. Field-effect
mobility, μFET, is in the 10-3 cm2V-1s-1 range (7.2 × 10-4 ± 4 × 10-4, averaged over 15
samples), while the on/off ratio and the threshold voltage are 204 ±91 and -0.03 ± 0.02 V
respectively. These data demonstrate how the P3HT EGOFET electronic performances have not
been significantly degraded by anchoring the PL bilayer. More importantly, gate leakage currents
are low being in the nA range that, along with the very low hysteresis exhibited by the double run
I‒V curves measured in PBS, show that the PL layer efficiently acts as barrier towards
semiconductor doping overcoming the already identified issue of EGOFET operating in PBS.[21]
Such a bio-electronic platform was subsequently used as sensing device. The binding of the
streptavidin (SA) protein to biotin was chosen as a testbed. Biotin is a small molecule with an
astonishingly high affinity (fM dissociation constant)[28] for the four binding sites of streptavidin or
equivalently, of avidin, both being tetrameric proteins. Accordingly, the electronic performances of
BIOEGOFETs prepared with biotinylated PL bilayers exposed to streptavidin solutions have been
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investigated. After the incubation with SA the device was first rinsed to remove unbound proteins
and finally measurements were performed in PBS electrolyte solutions. Representative results are
shown in Figure 2Figure 2a where the BIOEGOFET is exposed to 100 μg/mL (1.6 μM) of streptavidin in
PBS (10 mM, pH = 7.4). A sizable increase of IDS, when compared to that measured in buffer
alone, is seen with the fractional increase at VG =‒0.5 V reaching 60%. In this case the electrolyte
Debye length shortening in saline solution does not appear to impede transduction. Notably, a
comparable response is measured also in a 10-fold diluted PBS solution. While contributions can
be found dealing with OFET biosensing operation in an electrolyte solution,[18,29] to the best of our
knowledge, this is the first report of electronic (not electrochemical) biosensing performed in a
solution containing a physiologically relevant concentration of an electrolyte.
Figure 2Figure 2 a) Transfer characteristics of a BIOEGOFET with biotinylated PLs exposed to PBS 10 mM, pH7.4 (open symbols) and streptavidin (full symbols) solutions. A diagram for the rationale leading to the IDScurrent increase is provided in panels (b) and (c). In panels (d) and (e) negative control experiments areproposed. d) Transfer characteristics of a biotin-free BIOEGOFET exposed to PBS (open circles) and tostreptavidin 100 μg/mL (full triangles) are shown. e) Biotin-bearing BIOEGOFET exposed to bovine albuminserum 1 mg/mL (full diamonds) and to PBS (open circles) is shown.
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The sensing mechanisms leading to the observed current increase can be explained by
considering the binding of a negatively charged species (as streptavidin is at pH = 7.4) to a
dielectric interfaced to a p-type OSC. In such an EGOFET, a negative gate bias allows the
accumulation of anions at the electrolyte‒PL interface, while a capacitive coupling induces
positive charge accumulation at the OSC surface (Figure 2b). When the negatively charged SA
proteins bind to the biotin sites at the PL bilayer, they act as an extra (negative) gating inducing
more holes in the transistor channel (Figure 2c); the estimated charge that is added per unit
surface upon formation of the SA‒biotin complex, is -3.578 10-2 C cm-2.[30] Eventually, a
current increase is measured for a [PE-Q11:AU][PE-Q11:AU] Correct?Correct? clear capacitive effect, previously reported
also for the SA binding to a biotinylated p-type silicon nanowire FET.[31] As a further support to
the model, a charge density increase of ca. + [PE-Q12:AU][PE-Q12:AU] correct?correct? 9 × 10-2 C cm-2, [PE-[PE-
Q13:AU]Q13:AU] correct now?correct now? comparable to the estimated added negative charge, is seen already at VG =
0, namely just in the presence of the bound SA. Since the isoelectric point for SA immobilized on
PL monolayer is between 5‒5.5,[32] this detection scheme is expected to work at pH values larger
than 6.
Several control experiments were carried out demonstrating that the transistor response is
specific for SA-biotin binding. BIOEGOFETs bearing no biotin, do not, in fact, respond to the
loading with SA (see Figure 2d). This rules out any contribution of non-specific binding, and
demonstrates that the electronic response is actually due to the anchoring of SA to the
biotinylated PL. To evaluate the selectivity, bovine serum albumin (BSA) was assayed in the
presence of biotinylated PLs. BSA is a protein with a strong tendency to non-specifically adsorb to
surfaces. In Figure 2e the transfer characteristics of the BIOEGOFET, including the supported
biotinylated bilayer, exposed to a BSA solution (1 mg/mL) are compared to the response of the
lone buffer: BSA does not induce any significant variation. Therefore, the SA-induced increase in
IDS (Figure 2a) is the electronic transduction of the highly specific biotin‒streptavidin binding
event.
As a support to the BIOEGOFET unconventional approach, the selective protein binding to the
biotin moiety in the PL layer was further investigated by means of surface plasmon resonance
(SPR). SPR chips were prepared as the BIOEGOFET example and avidin binding was monitored
along with BSA for control purposes. The optimization of the capturing layer density was achieved
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by studying the coverage as a function of the surface density of biotin moieties (Figure 3Figure 3a). For
one biotinylated PL every 100 PLs the experimentally bound avidin surface coverage is 150 ± 20
ng/cm2 (2.2 ± 0.3 [PE-Q14:AU][PE-Q14:AU] correct now? correct now? pmol/cm2); this is in good agreement with the
theoretical coverage (1 [PE-Q15:AU][PE-Q15:AU] correct now? correct now? pmol/cm2) estimated assuming a PL head area of
0.7 nm2.[33] Further loading with biotinylated PLs, increases the avidin surface coverage that
eventually saturates at 270 ± 30 ng/cm2 (4.0 ± 0.4 [PE-Q16:AU][PE-Q16:AU] correct now?correct now? pmol/cm2). This is
close to the reported avidin full monolayer coverage on silica (8 [PE-Q17:AU][PE-Q17:AU] correct now?correct now?
pmol/cm2).[34] Accordingly, we have chosen a ratio of one biotinylated PL every 33 PLs for the
electronic sensing. A calibration curve showing avidin surface coverage (as probed by SPR) vs.
the avidin concentration is shown in Figure 3b. A limit of detection (LOD) of a few [PE-[PE-
Q18:AU]Q18:AU] correct?correct? nanomolar is associated with these measurements. In the same figure the
maximum BSA coverage of 20 ± 20 ng/cm2, is shown as a dashed line, indicating that the non-
specific binding is very low in the presence of the anchored PLs bilayer.
Figure 3Figure 3 a) [PE-Q19:AU][PE-Q19:AU] Please note that this f igure wil l be re-inserted by our typesetters in the nextPlease note that this f igure wil l be re-inserted by our typesetters in the next
step of processing so that none of the f igure is corrupted.step of processing so that none of the f igure is corrupted. The avidin surface coverage probed by SPR as afunction of the ratio between biotinylated PL and total PL. b) The avidin surface coverage probed by SPR asa function of the avidin concentration. The PL bilayer has a ratio of biotinylated PL/total PL of 0.03. c)BIOEGOFET response (fractional IDS increment) to streptavidin. Each data point is reported as the averagevalue along with standard error bar estimated over 15 replicates; the line is a logarithmic fit. The inset showsthe same data on a logarithmic plot. [PE-Q20:AU][PE-Q20:AU] Author please ignore this query. Typesetters: Please re-Author please ignore this query. Typesetters: Please re-
insert this f igure ensure that al l axes labels, numbers, and panel labels are not corrupted.insert this f igure ensure that al l axes labels, numbers, and panel labels are not corrupted.
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The electronic sensing analytical performances were also investigated. In Figure 3c the
responses (ΔI/I being the fractional IDS increases at VG = -0.5 V) of the BIOEGOFET to different
SA concentrations are shown. For each concentration, measurements were performed on 15
different devices and the average value and standard error (SE) are reported, the latter being
below 20%. The responses clearly scale with the logarithm of SA concentration over two orders of
magnitude and the limit of detection (LOD) is of 10 nM. The LOD was estimated as three times
the standard deviation (over 10 replicates) of the response measured in the PBS reference
solution (see the inset of Figure 3c). This allows label-free detection of biotin in the 10 nM‒1μM
range with a LOD of 10 nM. The responses are also fast as the IDS measurements are acquired
in 45 seconds. The comparison between SPR, a well assessed analytical tool, and the
BIOEGOFET platform shows that similar LODs are obtained. On the other hand, the BIOEGOFET
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sensors show performances two orders of magnitude better than those reported for the SA
electronic detection with carbon nanotube FETs (LOD = 2.5 μM).[35] BIOEGOFET sensors,
however, perform less well than the extremely sensitive biotinylated single silicon nanowires FET
whose lowest detection is of tens of [PE-Q21:AU][PE-Q21:AU] correct?correct? picomolar concentration).[31] However,
none of the previous determinations have been proven to deliver a reliable quantification, in a
large concentration range and, critically important, in a high ionic strength electrolyte solution.
Indeed, the BIOEGOFET platform, also matches the performances of customary [PE-Q22:AU][PE-Q22:AU] "label" label
needing" ? Please re-word this sentence.needing" ? Please re-word this sentence. label needing fluorimetric and spectrophotometric assays. In
particular, the LOD lies at the lower edge of the range of assays based on fluorescent biotin
analogues (LOD 30 nM),[36,37] that allow, however, for a much narrower dynamic range.
From an applications point of view, the proposed approach opens a wider perspective as
antibodies and proteins can be also bound to fluid phospholipid bilayers supported on solid
surfaces without altering the membrane properties.[38] The biotinylated PL bilayer anchored to the
OSC surface, can easily be further functionalized with virtually any receptors by using the well-
assessed biotin‒(strept)avidin chemistry.[28] In this respect, the SA-mediated binding of antibodies
to biotinylated-PL-supported bilayer was reported to provide efficient suppression of nonspecific
binding in an acoustic biosensor.[39] Furthermore, while the EGOFET sensors proposed to date
have had reasonable performances only in deionized water, the present BIOEGOFET works
efficiently in high ionic strength electrolyte solution, opening the possibility of detection in real
samples.
ExperimentalExperimental
Materials: Soy bean lecithin (EPIKURON 200) and N-((6-(biotinoyl)amino)hexanoyl)-1,2-
dihexadecanoyl-sn-glycero-3-phosphoethanolamine (Biotin-X DHPE) were respectively
purchased from CARGILL and INVITROGEN. [PE-Q23:AU][PE-Q23:AU] correct now?correct now? Poly-3-hexylthiophene
(P3HT), purchased from BASF (RR>98%, Sepiolid P200), was purified by successive Soxhlet
extractions with methanol and hexane.[40] All other chemicals were purchased from Sigma.
EGOFET fabrication: Si/SiO2 substrates with interdigitated gold source (S) and drain (D)
electrodes were cleaned using solvents of increasing polarity.[41] S and D were
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photolithographically defined (10 μm channel length and 10 mm channel width) by using vacuum-
deposited titanium as gold-adhesion-promoter layer. The purified P3HT chloroform solution was
spin-coated on the bottom-contact devices and subsequently annealed at 75 °C for 1h to improve
the OSC performances.[42]
PE-CVD coating: Plasma depositions were carried out in a home-build low pressure RF (13.56
MHz) plasma reactor described elsewhere.[43] Acrylic acid vapors (AA 99%, Aldrich, USA),
ethylene (Eth, Air Liquide) and argon (Ar, Air Liquide) were mixed before being let into the
reactor.[43] Conditions were: power 50 W, pressure 250 mTorr, flow rate of precursors: ΦAA = 2.5
sccm, ΦEth = 7.5 sccm, ΦAr = 2.5 sccm, deposition time was 3 s. PE-CVD conditions were
optimized to the best stability of COOH-functionalized coatings in water media.[44]
Vesicles preparation and PL layer deposition: soybean lecithin (4.5 mg),
phosphatidylethanolamine (0.5 mg), and the proper amount (50‒150 μg) of biotin-X DHPE were
dissolved in chloroform, then dried under N2 flow and kept for 60 min under vacuum. PLs were
rehydrated in PBS (1 mL), sonicated (10 min) on ice, and extruded through a polycarbonate filter
with 100 nm pore sizes using the Avanti mini-extruder (Avanti Polar).
Bio-conjugation: PL vesicles were immobilized onto PE-CVD-modified EGOFETs through the
formation of [PE-Q24:AU][PE-Q24:AU] correct now?correct now? amide bonds between the COOH surface groups and the
NH2 moieties on the polar heads of phosphatidylethanolamine. The EGOFET or SPR gold slides
coated with plasma-treated P3HT were incubated in a freshly prepared
ethyl(dimethylaminopropyl) carbodiimide (EDC) and N-Hydroxysuccinimide (NHS) solution (both
100 mM in PBS) for 1 h at room temperature, rinsed three times in PBS and immersed in the
vesicles suspension overnight under mild agitation at room temperature.
SPR measurements: SPR measurements were performed with a Biacore 3000 instrument (GE
Healthcare/Biacore AB). Substrates coated with lipids were glued with double-sticking tape in a
plastic frame of a Biacore 3000 chip cassette. BSA and avidin were immobilised by flow injection,
after docking the chip and performing a single prime operation to stabilize the surface in PBS. An
approximation that 10 resonance unit (RU) corresponds to 1 ng/cm2 of adsorbed protein was
used.[45]
BIOEGOFET electrical and sensing measurements: The BIOEGOFET current-voltage
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BIOEGOFET electrical and sensing measurements: The BIOEGOFET current-voltage
characteristics were measured using a semiconductor parameter analyzer (Agilent 4155C). A
gold plate (1 mm × 1 mm) in contact with a droplet (2 μL) of water or PBS was used as gate
electrode and the measurements were performed in a water-vapor-saturated environment. The
transfer characteristics (IDS vs VG) were measured keeping the drain voltage (VDS) constant at
-0.5 V. The transistor electrical figures of merit, namely the field-effect mobility (μFET), the
threshold voltage (VT) and on/off ratio, were extracted from the characteristics in the saturation
regime.[46] Sensing measurements were performed by measuring the BIOEGOFET transfer
characteristics in PBS (10 mM, KCl 2.7 mM, 137 mM NaCl, pH = 7.4). Solutions of SA (or BSA) in
buffer were placed on the S-D channel for 15 minutes. The channel was then rinsed with buffer to
remove the unbound proteins and finally the response was evaluated as the IDS relative current
increase at VG = -0.5V.
Supporting InformationSupporting Information
Supporting Information is available from the Wiley Online Library or from the author.
AcknowledgementsAcknowledgementsThe “Electrolyte-Gated Organic Field-Effect Biosensors- BioEGOFET” project, SEVENTHFRAMEWORK PROGRAMME - FP7/2007-2013 under Grant agreement no. 248728, and the“Gas Sensors on Flexible Substrates for Wireless Applications-FlexSMELL project, SEVENTHFRAMEWORK PROGRAMME‒PITN/2007-2013 under Grant agreement no. 2009-238454 areacknowledged for partial financial support. We also acknowledge funding from The Italian Ministryof Education, University and Research (MIUR) through PRIN project “Electronic andelectrochemical biosensors” 2009AZKNJ7. Dr. Francesca Intranuovo is acknowledged forperforming some PE-CVD deposition experiments. Henrick Toss from the University of Linkopingis acknowledged for supplying the photolithographic patterning of the S&D pads in the EGOFETdevices. Prof. Gilles Horowitz of LPICM, Ecole Polytechnique, Palaiseau, France, and Prof.Magnus Berggren from the University of Linkoping are acknowledged for useful discussions.
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